Abstract
An alternate treatment of the results of paper I is given. As in that paper, the Unruh boundary condition is formulated, the Unruh vacuum is defined as a state satisfying this boundary condition, and the thermal character of the state is exhibited. The present work differs in that it uses the double-wedge region of the Kruskal manifold and defines and uses a precise notion of distinguished modes.
| Original language | English |
|---|---|
| Pages (from-to) | 2520-2525 |
| Number of pages | 6 |
| Journal | Journal of Mathematical Physics |
| Volume | 27 |
| Issue number | 10 |
| DOIs | |
| State | Published - 1986 |
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